Senior Thesis GROUND WATER AND SUBSURFACE CONTAMINATION EXERCISES by John Mansperger 1994 Submitted as partial fulfillment of the requirements for the degree of Bachelor of Science in Geological Sciences at The Ohio State University Spring Quarter 1994 Approved by:
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Senior Thesis
GROUND WATER AND SUBSURFACE CONTAMINATION EXERCISES
by
John Mansperger
1994
Submitted as partial fulfillment of the
requirements for the degree of
Bachelor of Science in Geological Sciences
at The Ohio State University
Spring Quarter 1994
Approved by:
Page 2
Contents
Page
List of Figures 3
List of Tables 4
Chapter 1: Introduction and Basic Geological Processes 5
Chapter 2 - Unit A: Ground Water Basics 9
Chapter 3 - Unit B: Contaminants in the Subsurface 15
Summary 30
Appendix I: Exercises A1, A2, and A3, including answer keys 31
Appendix II: Exercises B 1, B2, and B3, including answer keys 42
Appendix Ill: Glossary 54
References Cited in Text 57
References Cited in Captions Only 58
Unit A
Figure 1
Figure 2
Figure 3
Figure 4
Figure 5
Figure 6
Figure 7
Figure 8
Page 3
List of Figures
Block schematic of typical sand and gravel units overlying bedrock
Block schematic of typical geological units in a glaciated area
Water table conformance to topography; capillary fringe
Recharge in highlands I discharge to lol/lllands
Recharge of contaminated water from surface water to well
Potentiometric surfaces in unconfined and confined aquifers
Cones of depression in unconfined and confined aquifers
Flow lines adjacent to an extraction well
Diagram of sources of ground-water contamination
Leachate plume distribution and movement below a landfill
Diagram of transverse and longitudinal dispersion
Concentration curves/fronts modified by advection & dispersion
Plume dispersion and development, intermittent slug dispersion
Advection only concentration vs. distance for continuous plume front
Plot of advection only concentration vs. distance for slug plume front
Development of plume and plume dispersion, continuous source type
Development of plume and plume dispersion, intermittent source type
Lagoon leakage plume and modified regional flow pattern
Figure 19 Cross section of regional ground-water flow illustrating hydraulic head 33
Figure 20a - c Graphical explanation of Darcy's Law utilizing sand-filled tube schematics 33
Exercise A1 I Part B
Figure 21 Oblique and transparent view of valley sediment geometry 34
Exercise A2
Figure 22
Figure 23
Figure 24
Exercise A3
Figure 25
Figure 26
Figure 27
Exercise 81
Figure 29:
Exercise 82
Figure 29
Figure 30
Exercise 83
Figure 31
Figure 32
Figure 33
Figure 34
Figure 35
Figure 36
Figure 37
Page 4
List of Figures, continued
Plan view of 3 well points with water elevation data.
Worksheet for Unit A I Exercise A2
Answer Sheet for Unit A I Exercise A2
Sample potentiometric map showing well point water elevation data
Worksheet for Unit A I Exercise A3; map of well water level data
Answer sheet for Unit A I Exercise A3; potentiometric surface sho1M1
Cross section of spill scenario described in Unit 8 I Exercise 81
Plan view illustrating plume size and shape fluctuations
Answer sheet for Exercise 82: plume size and shape fluctuations
Worksheet showing cross section of aquifer for Exercise 83
Answer sheet for Exercise 83: possible NAPL plume shapes
Small DNAPL spill, residual contamination
DNAPL plume penetrating into the water table
DNAPL through unsaturated zone, pooling on impermeable layer
Perched DNAPLs and pool with dissolved contaminants
DNAPL plume migration relative to surface spill area
List of Tables
Table 1 Table listing sources of ground-water contamination
36
37
38
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39
40
41
44
45
46
48
49
51
51
52
52
52
18
Page 5
Chapter 1: Introduction and Basic Geological Processes
Introduction to Units
The purpose of this senior thesis is to demonstrate the basic geological parameters
affecting the distribution and flow of ground water, and how these parameters interact with
subsurface contaminants. The units comprising this thesis contain exercises that are designed to
teach concepts used in ground water studies and remediation. The concepts are presented in tV'vQ
units that include a discussion of the concepts presented in each particular unit and related
exercises that illustrate those concepts. The exercises contain illustrations and tables, and are
characterized by simple maps and cross sections. Such information provides data for the
operation of formulas used in calculating various hydrogeological parameters and in VvQrking
through the exercises.
The overall object of the units is to show how ground-water and contaminant flow are
predicted, thereby providing a unified picture of the basic concepts in hydrogeology and ground
water pollution. Remediation methods will also be discussed. U.S. Environmental Protection
Agency (EPA) technology transfer handbooks and VvQrkshop and seminar summaries are used
as the basis of this VvQrk. This group of exercises is designed for second-year earth science
students and other professional personnel, such as managers, city council members, etc. The
exercises accompanying the units are in the appendices.
Discussion of Basic Geological Processes
Due to the limited ground-water resources in existence and the ever-increasing demand
for water, there is an urgent need to protect unpolluted ground waters, and to remediate (IM'lere
possible) polluted aquifers and soil. In order to predict the distribution and fate of contaminants,
much information must be knoll\11: the occurrence and distribution of ground water, the nature of
geologic materials and aquifer(s), boundary conditions, and confining units in the area of interest.
Ground-water contaminants and geologic materials vary greatly in their properties. In
this portion of the introduction, a brief overview of geologic processes IM'lich are limited to
materials, systems, and environments appropriate to this study are provided. Sediment-filled
river valleys have been a common location for agricultural, manufacturing, and transport
activities and communities. Many contaminant sites are located within this environment. To
support these activities water is withdrall\11 from aquifers in sediments or sedimentary rocks in
these valleys. In the same environments, potential contaminants are used and disposed of. The
other major groups of rocks, igneous and metamorphic, are not major water-bearing units. Water
and contaminant flow in these rock units is often confined to fracture channels. Flow in fractured
Page6
media is complex, difficult to sample and model, and beyond the scope of this v.urk. Thus it
deals primarily with sediments and sedimentary rocks.
Sedimentary rocks are composed of sedimentary particles derived from other rocks, or
compounds precipitated out of water by various processes or organisms. These sedimentary
particles, v.tlich vary in size from glacial boulders to fine oozes, are laid down (usually in a
horizontal orientation) in a sediment depositional system. Commonly, soils, poorly consolidated
sediments, and fragmented rock overlie bedrock. Sedimentary rocks are also composed of
sedimentary particles turned to rock by compaction, mineralogical changes, cementation, and
de-watering. Depositional systems vary greatly in their areal extent and v.urkings, and this
variation controls the properties of the sediments or the rocks formed from them. If the
depositional system of the rock or sediment is of limited areal extent, or characterized by
sediments of different sizes or properties, one v.uuld find the ground-water flow through such a
region to be more complex than that in a unit or series of units that \II/ere very homogeneous and
widespread. Sediments and sedimentary rocks can bury an eroded bedrock surface with lo\11/er
permeability and porosity. Determining the nature and configuration of that buried surface is very
important due to its effects on the movement of fluids in aquifers above it. Figures 1 and 2 show
examples of tv.u sediment depositional systems and underlying rock units. One can see that an
understanding of the nature and geologic history of an area aids in the characterization of a site's
hydrogeology. The characterization of a contaminant site in hydrogeological terms is paramount
in determining the extent of the contamination problem and the most effective and realistic
cleanup.
As noted above, most sedimentary rock units are deposited in overall horizontal layers
or beds. Subsequent ground-water flow through rock units tends to parallel the bedding planes, if
there is a noticeable difference in hydraulic conductivity (permeability) bet\11/een the units and if
the units remain horizontal.
The make-up and structure of contaminated geological materials are of major
importance in the determination of how those contaminants move and v.tlat eventually happens
to them. It is beyond the scope of this paper to examine geology, except as particulars in a
model site or to illustrate hydrogeologic principles. Geological conditions dealt with in this v.urk
have been chosen because they are typical, elementary, or best illustrate a particular concept.
The typical situation presented is one of unconsolidated sediments overlying sedimentary rock
units of varying permeability.
Page8
wen
Openlngs Largely Filled with Air
Figure 3: Water table typically mirrors the surface topography to some extent. Note detail of the capillary fringe (U.S. EPA, 1987).
recharge Area
Head decre..:oses Nitl depth
Discharge Area
Head increases with depth
Recharge Area
Head decreases with depth
Figure 4: Cross section through varied topography showng a high!and recharge area and a lower elevation discharge area. Ground-water flow paths are shown (after U.S. EPA, 1987).
\
Page 9
Chapter 2 - Unit A: Ground Water Occurrence in the Geological
Environment
Introduction
This unit investigates the occurrence and movement of subsurface water, and how water
in the subsurface is mapped. How geologic materials affect the occurrence of ground water, and
some ways that geological information can be presented are also discussed. The actual
exercises for Unit A are in Appendix I.
The Water Table
Most geologic materials contain voids or pores, and it is within these pores that ground
water exists and moves. Underground water occurs as soil moisture in the zone above the water
table, 'AA'lere the pores contain both air and water. This zone is kno\Nll as the unsaturated zone,
or sometimes the zone of aeration. In most areas there is a distinct water table, the upper
surface of the underground body of water in 'AA'lich all pore spaces are filled with water. The
unsaturated zone drains by gravity to the water table, but some moisture remains on the sides of
pores and between grains. This remaining water is kno\Nll as residual saturation and has effects
on the movement of contaminants and water through the unsaturated zone. The material just
above the saturated zone is saturated, but has a negative hydraulic pressure. The mass of water
in this thin volume is in place due to the wicking action of the pores of that geologic material.
This area is kno\Nll as the capillary fringe (Figure 3).
The water table generally conforms to the contours of the land surface. Gravity is
constantly acting to draw the water from "mounds" underlying high areas do\Nll to low areas,
leveling the water table. Recharge from rainfall and surface water bodies serves to replenish
water under the high areas (Figure 4). That the water table is not flat is due to the resistance to
underground flow of water by soil and rocks. The water table typically ranges from Oto 40 feet in
humid areas, and do\Nll to hundreds of feet in more arid areas (U.S. EPA, 1987).
The water table intersects the ground surface in swamps and is equal in elevation to the
water level in excavations (for quarries, highway borrow pits, or building foundations). The depth
of the water level in wells (usually given as an elevation above sea level, similar to land
contours) can also be measured. Surface bodies of water can show false water-table elevations
if affected by surface waters flowing into them (surface run-off) from a larger area of ground than
they themselves occupy. That is, if a stormwater drain from a parking lot empties into a pond, or
a river draining a valley empties into a lake, the water level in the pond or lake can be higher
than the adjacent water table. Under the driving force of gravity river or pond water will seep
do\Nll (infiltrate) through the underlying sediments or rock to the water table, . This seepage rate
Page 10
will often be slower, sometimes much slower, than the rate that run-off from the parking lot or
river refills the pond or lake. If the surface body of water is contaminated, the aquifer may also
become contaminated (Figure 5).
The water volumes (and levels) in surface bodies and aquifers fluctuate according to
recharge and discharge rates. Stream, river, and lake water levels are related to ground water in
that the water level in them can be above, level with, or below the water table. If the river or lake
bed is below the water table, typically due to erosion or a rise in the ground-water level due to
heavy rain or snow recharge the saturated zone discharges to those surface bodies of water.
Ground-water will seep up through the bed, or leak from springs along a riverbank or shoreline.
In the case of rivers and lakes, the level often depends on the influx of water from
creeks, streams, and other rivers. For an aquifer the levels change due to loss or gain from
surface bodies of water, infiltration of rainfall through the unsaturated zone, and through loss due
to drying of overlying soil and roots of vegetation. The term for the latter discharge path is
evapotranspiration. Knowing the locations and amounts of ground-water recharge and discharge
is important, because of the effects on the water table level, the dilution it causes in the ground
water, and the possibility of leaching contaminants from the surface or unsaturated zone.
Aquifers
A rock or sediment layer that transmits water at a rate fast enough to form a viable
source for use at a spring or \II/hen a well is drilled is knoV\11 as an aquifer. Layers or areas that
are nearly impermeable to water, or transmit it very slowly, are called aquitards. The term for the
ability of a geologic unit to transmit water is knoV\11 as permeability or hydraulic conductivity.
Units with low permeability or hydraulic conductivity do not allow water to pass through them as
easily as those with high permeability.
Ground water in aquifers occurs in tlll.Q basic scenarios: the unconfined aquifer and the
confined aquifer. The unconfined type is analogous to a kiddie pool filled with much sand and not
as much water. The ''water table" can be found by digging a hole or poking in a stick and seeing
how much length is wet, much like a well. The water surface (under the sand surface) is free to
rise and fall according to recharge and discharge. To use the same pool analogy to model a
confined aquifer, water could be added until it just covers the sand. A different, low permeability
geologic material is required to confine the water in the aquifer. An old plastic sheet with a few
tiny holes Ill.Quid be placed over the sand/water layer, and the pool filled to the top with silty mud
and allowed to dry. The sand aquifer is confined; very little water can flow upwards through the
plastic. If one was to stand atop the hardened mud and poke a tube (a "well") doV\11 through the
layers, including the plastic, the water Ill.Quid be forced up just a bit into the tube, above the level
of the plastic sheet due to one's body weight. This rise in the water level above the plastic layer
Page 11
represents hydraulic head or pressure. This analogy has some flavvs, the main being that true
hydraulic head comes primarily from the mounding in higher topographic areas, and from
recharge areas in the higher elevation of the confined aquifer (not just from a giant's
bodyweight). In reality, the weight of the overburden can add to the increased head. There may
be enough hydraulic head to force the water to the surface in what is called a flovving artesian
well, or to cause ground-water flow across aquitards (confining units) (Figure 6).
Ground-water Movement
The water table height in confined aquifers is actually a potential height to which the
ground water v-.uuld rise in a well or pit if not confined by the overlying confining unit, such as
water freed by drilling a well. This potential height (pressure) exists everywhere in the confined
aquifer and is knoVllll as the potentiometric surface. Wells show hydraulic pressure (knoVllll as
head) much like a giant pressure gage. This hydraulic pressure, due to gravity acting on water in
higher areas of the aquifer, is responsible for the movement of ground water; it is the driving
force.
As stated before, all geologic materials pose some impediment to the flow of water
through them, due to frictional fluid forces and convoluted flow paths around grains and through
pores. If flow were very fast, the mounding effects and variations in the potentiometric surface
v-.uuld not be seen. Fractures in rocks can act as conduits for ground-water flow, and this effect
can be very important to overall flow patterns, offering relatively unimpeded flow paths.
However, this flow is very complex.
Advection
Advection is the hydraulic principle governing ground-water flow. Advective flow is the
product of several parameters, which are expressed as Darcy's law, Q = KIA. It states that the
flow rate through any porous medium is 1) proportional to the pressure driving the flow (head},
2) inversely proportional to the length of the flow path, and 3) affected by the hydraulic
conductivity of the porous medium (geologic material). Exercise A 1 deals vvith practical
application of Darcy's Law describing flow per unit area.
Geometric Changes to the Potentiometric Surface
When a well is drilled into an aquifer, a casing pipe is installed to keep equipment from
being damaged and to allow pressure or suction to be applied to the area near the bottom of the
well. The casing has holes in it in this section. This is called the screen, and this area provides
access to the geologic materials (aquifer) outside of the well in a controlled manner. A water well
is drilled until it has penetrated the water table or potentiometric surface of the particular aquifer
desired. Water is vvithdraVllll by pumping and water from surrounding parts of
Figure 5:
Figure 6:
Page 12
Diagram shov..1ng how contaminated water from a surface body can be induced to flow into ground water, and subsequently the v..1thdrawal well, by pumping (U.S. EPA, 1987, from Miller, 1980).
Aquifer A is unconfined and aquifers Band Care confined, but may leak through confining units to recharge adjacent water-bearing zones (U.S. EPA, 1987).
Page 13
the aquifer flows towards the well to replace that INhich is pumped out. Wells that remove water
from an aquifer (pumping or Vllithdrawal wells) modify the potentiometric surface and affect
ground-water flow patterns. The surrounding flow is necessarily modified because water now
flows towards the well to replace that INhich is pumped out. What is knovvn as a cone of
depression forms around the well in the potentiometric surface (or water table) (Figure 7).
The size and shape of the cone of depression depends upon the Vllithdrawal rate, the
hydraulic conductivity of the surrounding rock or sediments, and the period of Vllithdrawal. The
hydraulic head is lowered locally for Vllithdrawal wells and equipotential lines in the vicinity show
a characteristic series of concentric contours indicating the Vllithdrawal area. Flow paths or flow
lines are lines dravvn on maps and cross sections depicting the direction of flow that individual
water "particles" travel underground. Figure 8 shows typical flow paths in the vicinity of an
extraction well. Flow paths, INhich necessarily cross equipotential lines at right angles, are
diverted towards the Vllithdrawal area. The situation is different for wells adding fluid to the
subsurface. An injection well is one in INhich water is introduced under some type of pressure, by
means of a well casing Vllith either the water level maintained above the potentiometric surface,
or by active pumping. Here the effect on the potentiometric surface is opposite: the
potentiometric surface is raised above the surrounding areas. This is a case of highly localized
recharge, and water immediately begins to flow away from this area due to the new hydraulic
gradient. Of course, the flow rate and direction are affected by the hydraulic conductivity of the
aquifer unit being injected and by any preferential, anisotropic effects of the sediments or rock.
This ability to manipulate the potentiometric surface and subsequent subsurface flow using both
Vllithdrawal and injection wells represents a major tool to be used in the control and cleanup of
subsurface contamination.
Geologic Information
Information on geologic conditions in the subsurface is presented in a variety of ways,
some of INhich is used in the educational units developed in this thesis. When drilling a well, the
drill bit passes dovvn through successive layers of soil and rock. A detailed record of the types
and thicknesses of sediments or rocks encountered is made at that time. This record, a well log,
can be augmented by putting a great variety of instrumentation dovvn the borehole during or after
drilling. Special devices can be used to retrieve samples of the geologic materials at various
levels or any of fluids encountered. These samples can be very important in quantifying the
hydrogeologic properties of the area under study. They provide hard data for the operation and
checking of theoretical and laboratory models of ground-water and contaminant flow. The data
gathered can be used to create a cross section of the area. Cross sections show an elevation
(sideways) view of the layers and underground structure of an area. Some of the previous figures
have been cross sections. They show the subsurface in a sideways view, similar to a cake slice.
I /
·Confining Bed
~Flowlines
I I I I
Page 14
Land SU"ace
--..... .:: -=-........... - - &
?''' Dralllidown \ \
Confining Bed
o--~
c----~
o---~ Confined Aqu~ ~--~
- - -: :;.=---=-.,. ,,.,.-
/ ~Coneof
/ Depression
~-o
,.._ ----o
~---o
~----o
Confining Bed
The cone of depression surrounding a pumping well in an unconfined aquifer is relatively small COIT1J8red to trat in .a confined system.
Figure 7:
Figure 8:
Cones of depression in a) confined and b) unconfined aquifers (U.S. EPA, 1987, from Heath, 1983).
MODERATE
FAST /
MODERATE
Flow line generated by an extraction well (U.S. EPA, 1989).
Page 15
Chapter 3 - Unit 8: Transport and Fate of Ground-Water Contaminants
Introduction
This unit investigates the occurrence, types, and sources of contaminants. Transport of
contaminant in the subsurface and dispersion and diffusion phenomena are also discussed.
Finally, contaminant isolation and remediation strategies are introduced. The exercises for Unit B
are located in Appendix II.
Types of Contaminants
Virtually any toxic or usage-limiting chemical or compound, either created by humans or
occurring in the natural environment, has the potential to contaminate ground v.ater, not just
those caused by such site-specific incidents as leachates from landfills or surface spills.
Contaminants cause v.ater to become "polluted" Ylklen the contaminant concentration increases
above a certain level (a quality standard set by agencies and/or law). Human activities can cause
the migration of natural contaminants (such as highly mineralized or saline ground v.ater) into
previously uncontaminated aquifers.
Contaminants are of three basic types: physical, chemical, and biological. Physical
contaminants (those Ylklose chemical interactions are not of primary importance) include
radioactive particles (isotopes) and asbestos. Metal ions, the most dangerous being the more
toxic "heavy metals," are included in the second basic grouping of contaminants: chemical. This
is the most diverse and prevalent contaminant group. Industry brings new chemicals into
widespread use every year, so the list of potential contaminants continually grows and evolves.
Chemical contaminants can be categorized further: metal ions (mentioned previously), acids and
alkaline substances, ionic compounds, and organic chemicals, including petroleum-based fuels.
This sub-group, the organics, is very complex and diverse. Included here, besides fuels and oils,
are organic solvents (eg. benzene), pesticides and fertilizers (nitrates), chlorinated solvents and
compounds (including PCBs), and complex compounds such as dioxins and furans. The last
basic type of contaminant is biological: bacteria and viruses that survive in the subsurface and
that can cause harm to humans.
Contaminants can be in their pure form (free-product phase) or dissolved or entrained
into ground v.ater (U.S. EPA 1987)
Nonaqueous-Phase Liquids
A special group of organic chemicals exists: nonaqueous-phase liquids (NAPLs). These
are hydrocarbon contaminants Ylklich do not mix with v.ater, but yet are mobile in the subsurface.
These compounds have recently been recognized as a major problem in the effort to clean and
Page 16
protect many aquifers (U.S. EPA, 1991). Complicating the problem is the fact that soluble
portions of NAPLs dissolve into ground water, contaminating it. However, this diffusive process
takes time and much of the liquid remains in a separate phase having very different properties
from water. In this manner it acts as a reservoir for continued contamination of associated
ground-water. NAPLs that are less dense than water, light nonaqueous-phase liquids (LNAPLs),
Vl.111 float on top of the water table. Dense nonaqueous-phase liquids (DNAPLs) are more dense
than water and wll penetrate and sink into the water table if sufficient quantities accumulate.
NAPLs present serious problems for both the detection of contaminants and cleanup
(remediation) of an aquifer and/or the unsaturated zone above an aquifer.
DNAPLs present an especially tough problem that is now being recognized at many
contaminant sites that have been undergoing cleanup for some time. DNAPLs can become
immobile in the subsurface, yet continue to contaminate ground water for centuries (U.S. EPA,
1991). Immobilization occurs by partitioning onto organic solvent or materials. Initial efforts at
many sites were not designed to detect DNAPL contaminants, yet they are often present and
remain the source of continuing ground-water contamination (U.S. EPA, 1991). DNAPL
movement in the subsurface is very much controlled by forces different from those controlling
dissolved-phase contaminants and ground water. Capillary forces and the distribution of these
forces in geologic materials exert a far greater effect on them. Even marginal remediation of
DNAPLs requires more detailed information on these properties than for other contaminant
materials. However there is a risk that DNAPLs wll spread contamination further during site
evaluation (drilling and sampling). No proven technologies able to completely clean up aquifers
contaminated VI.1th DNAPLs completely, and containment is the primary, realistic goal in these
aquifers (U.S. EPA, 1991).
Sources of ground-water contamination
Contaminants can be released into the environment by design, through ignorance or
neglect, or by accident. Figure 9 shows common sources of ground-water contamination. These
can be studied in a frame'M>rk of 6 categories as detailed in Table 1 .
. Contaminant Transport
Flow of many ground-water contaminants is controlled predominantly by hydraulic
pressure and by density. Mixing characteristics of contaminants in water and wetting/capillary
interactions VI.1th geologic materials are also important. Permeability and the wetness of those
geologic materials also contribute to the net movement of a contaminant. Capillary action and
gravity draw a spilled contaminant into a soil Vlklere the contaminant begins to fill soil pores.
Some is trapped as the contaminant moves do'Mlward, displacing soil gas (liquids are denser). If
--~--~---Percolation
I I t •
,~
Discharge or Injection
" ....
Page 17
Water Table 1 -------- -1- ------
Percolation I t /
Confining Zone
Artesian Aquifer (Fresh)
Artesian Aquif8' (Saline)
----Intentional Input
+ ___ Lnntentional
~ - Ground-Water
Movement
Figure 9: Methods of contaminant release. Dotted arrovvs show unintentional movement of contaminants. Heavy dashed arrow shov.s intentional input to the environment. Solid arrows show general ground-water movement. (U.S. EPA, 1987, from Geraghty and Miller, 1985).
Page 18
Table 1: Sources of ground-water contamination. (U.S. EPA, 1987, from OTA, 1984).
Category I-Sources designed to discharge substances
S~bs~rface percolation (e.g .• septic tanks and cesspools) ln1ectron Wells
Open burning and detonation sites Radioactive disposal sites
Category Ill-Sources designed to retain substances during transport or transmission Pipelines
Hazardous waste Non-hazardous waste Non-waste
Materials transport and transfer operations Hazardous waste Non-hazardous waste Non-waste
Category IV-Sources discharging substances as consequence of other planned activities Irrigation practices (e.g .. return flow) Pesticide applications Fertilizer applications Animal feeding operations De-icing salts applications Urban ruhnoff Percolation of atmospheric pollutants Mining and mine drainage
Surface mine-related Underground mine-related
Category V-Sources providing conduit or inducing discharge through altered flow patterns Production wells
Oil (and gas) wells Geothermal and heat recovery wells Water supply wells
Other wells (non-waste) Monitoring wells Exploration wells
Construction excavation
Category VI-Naturally occurring sources whose discharge is created and/or exacerbated by human activity Groundwater-surface water interactions Natural leaching Salt-water intrusion/brackish water upconing (or intrusion and
other poor-quality natural water)
Page 19
enough compound was released, it will reach the water table. Here soluble compounds begin to
dissolve into the ground water. Less soluble compounds either spread out over the surface of the
water table (if they float on water) or start to sink and penetrate the water table. If smaller
amounts of contaminant is released, or the water table is far below the ground surface, the
contaminant may not reach the water table. This is due to sorption onto and coating of the
unsaturated-zone materials and trapping of some portion in soil pores. These processes can
reduce the amount of contaminant in the mass as it seeps do'Mlward.
Movement of Contaminant Plumes
Three general processes act on chemical contaminants in ground water. They are
advection, dispersion, and retardation. Advection was discussed in Unit A Vlklen basic ground
water flow was described, along with Darcy's Law. Dispersion is the spreading out of a
contaminant plume due to irregular flow and mixing. Retardation is the slowing of a contaminant
plume by any one or more mechanisms.
Advection of Contaminant Plumes
Advection is the term used to describe both ground-water movement and the transport of
a nonreactive, conservative compound at the average velocity of surrounding ground-water flow.
One method used to measure velocity (and also direction) is to introduce a tracer of some sort
into a well and measure how fast (and perhaps Vlklere) it moves. There are many types of tracers
(including contaminants themselves) and many tracing methods. Simple methods include
measuring how fast a tracer is carried out of a well by ground water flowing by and through the
well. Or, a series of surrounding wells can be drilled into the same geologic units and then
measured by the time it takes for the tracer to travel to another well. This method indicates the
direction that ground water is flowing.
Figure 10 shovvs a contaminant plume from a leaking waste disposal lagoon being
moved along with the regional flow of ground water. The equipotential lines and flow path arrovvs
are sho'Ml. Note that the lagoon contributes to the aquifer flow and that the river gains water
from the aquifer, Vlklich is contaminated in this case.
Dispersion of Contaminant Plumes
Dispersion in hydrogeological terms is the group of forces acting to dissipate, or to thin
out a contaminant mass in the subsurface. Dispersion occurs in all directions and can be
affected by the properties of the geological material. It is caused primarily by the differences in
velocity found in a pore channel. The same effect is seen in a pipe transporting fluid, such as a
water or steam pipe. If the flow is measured at various points across a cross section of the pipe,
Page 20
760 230
740 ---=-----------_]225 j ..91!
.~ ! 700 1ii QI
~A .,
I 680 Sand
660
0
100 200 (meters)
200 400 600 (feet)
Horizontal Scale
\. ~ ......... Chloooe concentration, mg/I
a Standpipe tip
o Piezorneter tip
Multi-ievel sampling po;,t
Y WatS" table
r?ZJ Clay
~ Flow direction
Figure 10: Plume of leachate migrating from a sanitary landfill on a sandy aquifer shoVlling highest contaminant concentration at the center of the plume (U.S. EPA, 1987, from Freeze and Cherry, 1979).
Mean Flow
Microscopic scale of a granular medium
Figure 11: Diagram of transverse and longitudinal dispersion at the microscopic level particle paths in matrix shoVlling longitudinal & transverse diffusion plume (U.S. EPA, 1987, adapted from Freeze and Cherry, 1979).
200
Page 21
flow is found fastest at the center and slovver closer to the pipe wall (side of the pipe). This is
due to drag effects betvveen the pipe and fluid. The same effect occurs in pores in geological
materials, \/Vhich can have any number of shapes.
The slolNing of only part of the flow relative to another creates no effect \/Vhen the
transported fluid is just ground water. Hovvever, \/Vhen a contaminant is mixed VI.1th the water, the
net effect is dispersion. Some of the contaminant gets positioned in the flow adjacent to a pore
wall, llVhile the now-reduced amount forges ahead INith the fastest water flow. This process tends
to spread the plume out along the axis of general flow--longitudinal dispersion (Figure 11 ).
Contaminant plumes disperse in a direction transverse to flow by several mechanisms.
The most important is caused by the convoluted flow path taken by all fluids around the grains of
the material through llVhich it is floVIAng. These pathways as a \/Vhole add up to the general flow
direction. But some water and contaminant "particles" take very tortuous flow paths. The velocity
of some portions of the flow is slovver than others, and the net result of this is the same:
dispersion of the contaminant mass.
Dispersion of contaminants must always be considered along VI.1th advection \/Vhen trying
to determine the transport of a plume of contaminants. Geologic materials (the soil and broken
rock near the surface, as vvell as bedrock and aquifer materials) contain pores of a variety of
shapes, sizes, and relative position. Pores that are not round can be oriented in a preferential
direction, depending on the geological forces that emplaced the materials.
Another method of dispersion is diffusion, the tendency for concentrations of compounds
in solution to spread out and equalize the overall concentration. All methods of dispersion tend to
reduce the concentration of an advecting plume. The effect at a monitoring vvell doV1111gradient
from the source is not one of a massive increase in contaminant concentration from zero to the
maximum as the plume front arrives, but instead is a curve increasing to a maximum. This curve
is called the breakthrough curve and is illustrated in Figures 12 and 13 (a and b). These are plots
of contaminant concentration at increasing distances from the source. The second set of graphs
shows a plot of a one-time release (a slug). Two different time periods are shoVllll illustrating the
cumulative effect of dispersion over longer and longer distances. Note the typical bell shaped
curve. Refer to Figures 14 and 15, llVhich illustrate contaminant fronts unmodified by dispersion.
Some typical actual plume shapes are shoVllll in Figure 16 (a and b), and in Figure 17.
The movement of both ground water and contaminants is controlled by the same
factors: gravity, the permeability and vvetness of the geologic materials they come into contact
VI.1th, and how miscible (soluble) the contaminants (or components of a complex contaminant, eg.
gasoline) are in ground water. Any liquid has a density greater than air and VIAii displace the gas
component in the unsaturated zone.
Page 22
Distance ___ __....,..~
Figure 12: Plot of contaminant concentration versus distance from contaminant source sholfving the movement of a concentration front by advection and modified by dispersion (from U.S. EPA, 1987).
Time Period A
Time Period B
Average Flow
•
f¢: Advection
I Component Only
Figure 13: Plots of contaminant concentration versus distance from contaminant source for a
dissolved contaminant slug showng movement by advection and the change in
plume shape due to dispersion. Note that dispersion increases over time and
therefore distance from the contaminant source (from U.S. EPA, 1987).
Page 23
lllilll ::~::· Dissc>Ned ConstitUent ,,,,
0 •• ,
Average Flow .. Distance-->-
Figure 14: Plot of contaminant concentration versus distance from contaminant source sho>Mng the movement of a concentration front by advection only (from U.S. EPA, 1987).
Average Flow ... Distance ~
Figure 15: Plot of contaminant concentration versus distance from contaminant source for a dissolved contaminant slug showng movement by advection only(from U.S. EPA, 1987).
Page 24
A. The development of 1 contamination plume from I continuous point eource.
Flow.
B. The travel of a contaminant slug(s) from a one-time point source or an intermittent source.
f 0 0 0
Figure 16: Effects of continuous and intermittent sources on plume shapes as affected by dispersion (U.S. EPA, 1987).
Monitoring WeD.
11--1-./~ I /-/-
Leaky Lagoon r Water Table
Alluvium / Bedrock Contact
River
Figure 17: Effect of leakage from a lagoon on a regional flow pattern; typical plume migration path is shoW'l (U.S. EPA, 1987, from Geraghty and l.!iller, 1985).
Page 25
An initial spill of a hydrocarbon is wicked into the soil by capillary action and gravity. Air
must be displaced until the water table is reached. Highly miscible materials dissolve into the
ground water right away, VIA'lile less miscible materials float and spread laterally or tend to
penetrate the water table. In all cases the ground-water flow will tend to entrain the contaminant
(through hydrodynamic and viscous forces) and move it downstream.
Retardation
Movement of contaminants in the subsurface can be slowed down by a number of
chemical and physical processes. They retard or delay the migration, sometimes substantially,
relative to surrounding water underflow. These processes can be broken down into four
categories: dilution, filtration, chemical reactions, and transformation. The first category includes
dispersion, VIA'lich can break up a slug of contaminant and cause intermixing with water. The
reduced concentration may be below the contamination-problem threshold at a point of usage for
the aquifer water. Diffusion gradients, a type of dispersion, are reduced VIA'len contamination is
diluted. Filtration is relatively simple in operation: contaminants become trapped in smaller pore
spaces. The latter are the same flow paths that allow advection and thus may clog up over time,
reducing flow.
Ion exchange, the exchange of ions of a contaminanUground-water solution with
geological materials present in the subsurface, is a very important retardation process. Ion
exchange can remove contaminant ions from the flow, only to release them later if chemical
equilibrium conditions change. This is usually controlled by changes in pH (U.S .. EPA, 1987).
The geological materials present a limited number of exchange "sites" on molecules, and these
can be exceeded over time by continuously refreshed leachate. When the capacity is exceeded,
contaminant ions begin to move freely.
Transformation mechanisms of retardation include volatilization, VIA'lere parts of the
contaminant change from the liquid to the gaseous phase. This can reduce the viscosity of a
contaminant also. Contaminants can also be affected by microbal activity in the subsurface,
kno'Nledge of VIA'lich has only recently come to light (U.S. EPA, 1987). Biotransformation can
degrade a contaminant to another compound, with a different mobility and characteristics.
The effects of retardation on a complex contaminant plume leaching from under a waste
pile is illustrated in Figure 18. Monitoring wells are shown placed at increasing distances form the
pile, down into the plume area. The sketch is of conditions at one particular moment in time.
Compounds with higher retardation rates for the specific conditions under the site have not
traveled as far as those with lower retardation rates.
Page 26
Contaminant Isolation and Remediation Strategies
The ideal goal \Mluld be to clean up every contaminant site to the degree that it was
indistinguishable from a virgin site. No evidence of contamination \Mluld then be detectable
through investigation or through effects on the environment or humans. This is impossible, not
only because of technical limitations, but also due to limited fiscal resources. Often a site must
be viewed in the continuum of Wiat it was used for, how much income was generated during its
use, and Wiat the cost benefits of varying degrees of remediation versus the (and aquifer's)
future value (a broad term here) of the site and aquifer \Nill be. Parties found legally responsible
have finite resources and the government makes up the difference Wien the cost of dealing \Nith
the problem exceed those resources. The government and society also have finite resources,
generated by taxes and loans to be repaid INith future taxes.
The realistic goal is to contain (isolate) and/or treat (remediate) contaminated ground
water, and to clean (or partially clean) contaminated aquifers deemed of high economic value.
Ground water and contaminants can be extracted and treated by physical, chemical, or biological
methods on the surface or in-situ (in place underground) by chemical or microbal methods. This
section provides an overview of all processes, INith a more detailed analysis of physical
containment and remediation techniques. The source materials used for this thesis emphasize
hydrocarbon contaminants, and that bias is reflected herein.
Hydrocarbon Contaminants: Physical Processes
An obvious first step towards remediation, after site characterization and study, is to
prevent or slow the spread of contamination. This can be viewed as a step-by-step process,
starting at the mechanism for contaminant release. If a leak is responsible for the release, it is
stopped by repair or transfer of materials. Leaking barrels are removed and leaking lagoons
pumped out. If significant amounts of contaminant are present in near-surface soils and these
are infiltrating the ground, they \Mluld also be removed. Another approach is to prevent further
infiltration into the subsurface by controlling infiltration of surface water. This is done via
impermeable barriers on the surface, planting vegetation INith high evapotranspiration rates, and
controlling surface flow on the ground and into bodies of water, through contouring the surface
(grading) or digging surface collection trench systems.
Once the contaminant has migrated into the subsurface, the strategy of containment is
employed. The first type of containment consists of installing an underground barrier highly
impermeable to the contaminant plume, a type of curtain. These barriers, of clay, metal, or
polymers, ideally block any migration route in the subsurface. Sometimes these barriers can be
"locked into" an impermeable layer below the site, preventing flow underneath them. If that
option is not available, due to deep or nonexistent boundary layers, these barriers, may still be of
Page 27
use to prevent migration of contaminants and vapors in the near surface. Subsurface barriers
can be thought of as hydrostatic controls, as compared to active pumping (hydrodynamic)
controls. Barriers can be used along with hydrodynamic controls to make the latter more
effective.
The above options of removal, surface infiltration control, and barriers all have
limitations, such as high cost or unavailable materials, lack of acceptable dumps (or transport to
them), and the inability to verify the integrity of subsurface barriers.
The last method of containment is through hydrodynamic control of the contaminant
plume relative to the pre-existing site flow conditions. The goal is to isolate the plume from other
uncontaminated waters or flow, and to prevent further movement of the pollutant(s) through the
subsurface. A series of injection \/\/ells up gradient (upstream) from the plume inject
uncontaminated water at a rate high enough to overcome the ground-water flow (hydraulic)
gradient into the zone of contamination. The water to be injected is withdrawn from areas
adjacent to the plume, but far enough away so that contaminated water is not drawn into these
\/\/ells. This approach requires thorough knollllledge of flow parameters in all surrounding
materials, and plume location and extent; it also requires careful operation of the system. This is
an active system that requires continuous monitoring and po\/\ler input for as long as the plume
remains.
Withdrawal and Treatment
This technique can involve withdrawal \/\/ells, or both injection and withdrawal \/\/ells (or
buried trenches as in Figure 19. The latter approach could be considered an elaboration of
hydrodynamic containment. In simple withdrawal, contaminated water (or pure contaminant) is
pumped to the surface for treatment. Surface treatment options are quite varied and are not
discussed in this IM'.>rk.
In injection/withdrawal systems, \/\/ells down gradient from the contaminant plume
withdraw water \/Vhere it is delivered to some type of treatment system \/Vhich removes
contaminants. This water is injected through \/\/ells up gradient of the plume, accomplishing tlM'.>
tasks. The water is injected at a rate high enough to overcome the hydraulic gradient into the
zone of contamination, forcing the pre-existing flow around the plume. Much of the injected
water flows into the plume area and begins flushing the plume from aquifer materials, beginning
the remediation of contamination. The definition of withdrawal and treatment technique could
also be applied to the extraction of soil contaminant gases.
Figure 18: Cross section of typical waste pile showng distribution of contaminants wth different retardation factors in the aquifer materials. The contamina.1t that has spread the most is the least affected by any retardation (from U.S. EPA, 1989).
::: · ~ ::: i.,; o.t~ . 'ta.\.\e
Page 29
DNAPLs present special problems to remediation and special dangers to the
environment when present. Physical removal via pumping, trenches, vacuum extraction of soil
gas, soil flushing, physical barriers, and the use of hydrodynamic controls is used to control
DNAPL contaminants.
In some cases the contamination of an aquifer or at a site may be so wdespread or so
difficult to reach and remove that cleanup is not possible and containment is the only approach.
Even containment cannot be assured by using subsurface barriers and hydrodynamic controls in
other areas. These areas are affected by widespread contamination, fractured bedrock, or
regional underground stream systems (U.S. EPA, 1989). In these cases the entire aquifer is
sometimes made off-limits to withdrawal by pumping through code restrictions on water wells.
Affected peoples and businesses are provided with alternate sources, through extended water
supply piping systems. The factors that are considered when making the judgment for either
containment alone, or including cleanup, have been discussed at the beginning of this section.
Soluble Contaminants
Soluble contaminants dissolve in ground water and do not become immobilized as
readily as many hydrocarbon contaminants. Common methods of remediation are the same as
those utilized to treat ground water contaminated with the soluble components of hydrocarbons,
which are covered in the previous section. Aquifer flushing is often used, with the chemistry of
the flushing water adjusted to facilitate mobilization of all the pollutant.
Page 30
Summary
The U.S. EPA booklets and manuals provide a good starting place for the generation of
educational materials regarding hydrologic principles and the transport and fate of subsurface
contaminants. These manuals contain materials for VIAlich additional exercises could be
generated. For example, an exercise combining equipotential maps and flow paths could be
integrated into a scenario VIAlere changes are made to the potentiometric surface and
contaminant flow paths are modified. The source materials provide numerous site examples
VIAlich could be reVl.{)rked into additional exercises.
Page 31
Appendix I
Exercises for Unit A
Page 32
UNITA
EXERCISE A 1 : Ground-water Flow Rates
Introduction In this exercise you will examine how hydraulic head and ground-water flow are
interrelated and will calculate flow through a confined aquifer of simple geometry. The Darcy flow equations govern flow in this instance. Part A of Exercise A 1 presents the concepts; Part B is the exercise containing actual calculations.
Supplies and Equipment Required Calculator, notebook paper
Objectives Review the relationship betV11een hydraulic head and flow direction in Unit A.
Calculate the flow through a confined aquifer using data from tv-.u observation VI/ells.
Tasks Part A:
Darcy's Law is the basic expression used to describe fluid flow in aquifers. It can be modified in a number of ways to account for different flow situations, but in its basic form (sho\Ml below) it calculates the quantity of fluid flow per unit area (across the direction of flow). Darcy's Law. Q = KIA [flow per unit area]
Where Q =quantity of flow per unit time K = hydraulic conductivity of the aquifer, in gal/d/ft2 I = hydraulic gradient (hydraulic head), in feet per foot (fUft) A = cross-sectional area through which the flow occurs
The equation takes into account the resistance that the aquifer poses to flow, the pressure on the fluid (hydraulic head}, and over how much area this hydraulic gradient can act. An example of how hydraulic head affects the fluid flow direction is sho1M1 in the 3 schematics in Figure 20. They represent sand filled tubes: confined aquifers with a cross-sectional area of A. The ends are constructed so that water can be forced in one end and the resulting flow amount measured at the other end. The tubes have a pair of flexible hoses connected to the sides, one near each end, L feet apart. These tube will be used to measure the hydraulic head at the points where they connect to the aquifer tube, much like observation VI/ells in a real aquifer.
Figure 20a shows a tube in a horizontal position and a quantity of fluid per unit time is made to enter the tube. The water can be considered incompressible and flows through the sand and out the other end. The water level rises in the hoses in response to the force being applied to the water to push it through the sand. Energy is expended moving the fluid through the sand and this shows up as a lo\lller hydraulic head measured in the do1M1stream measuring hose. The difference in head (H) along the flow path length (1) is the hydraulic gradient and is expressed as H/L. If the flow (Q) and area (A} are constant, but a different aquifer material is present, say with a loV11er hydraulic conductivity, the head loss will be greater. Flow is in the direction of decreasing head.
Figure 20b shows tubes oriented vertically. In one case, water is being forced up through the tube from below. The hydraulic head will always decrease in the direction of flow, and the measuring hose upstream (to the flow direction) show a higher hydraulic head. In the other situation, flow is seen form the top dolMl, and the hydraulic heads in the measuring hoses are reversed. The measuring hoses are like a pair of VI/ells in the field, one drilled to a shallow depth and the other drilled deeper. This scenario is illustrated in Figure 20c, which shows the water levels in 3 sets of VI/ells located in a recharge area, an area of horizontal flow, and an area of discharge.
~ 3 Pairs of Wells ------/ Shallow Wei~ c;ep Well (typ.) ~ Discharge Area:
upwo..r-4 ~tic.crl .}°: \,...,
'(_ Water Levels Shaded JI !
/ (typ.)
·''
·---II'"
----------
_V -·-
Horizontal Flow Lines
Figure 19: Cross section diagram of hypothetical regional ground-water flow. Water levels of pairs of wells illustrate the hydraulic head driving the flow. (from U.S. EPA, 1987).
A. 1-\or\""t. .:>v..'r-o. ~ H f So. V'-~-fi \\ c ~ tu,;;...\:...=e.. _ _..i....L.-----J..,..1..--.
Gradient = HI L = I, the energy required to move the water distance L a = Quantity of flow, gpd A = Cross sectional area of flow, ft2 K = Hydraulic conductivity = gpd/ftZ
a
B. Vertical tube with flow from bottom to top.
C. • Vertical tube w:th flow from top to bottom.
Q Q
T L
......____.l
A A a
Figures 20a, b, & c: Sand-filled tubes illustrate Darcy's Law and the relationship of hydraulic gradient to flow direction. (from U.S. EPA, 1989).
Page 34
Part B: In the follo'A1ng example (adapted from U.S. EPA, 1987) you will use Darcy's Law to
calculate the underflow (underground flow) in a confined sand aquifer. Parts of the cross-section of a sediment-filled valley are showi in Figure 21 IMlere they intersect with M.o observation wells. They are located one mile (5,280 ft.) apart, one directly up-flow from the other. The aquifer is confined by glacial till with a surface that is essentially flat, as are all bedding planes and unitto-unit boundaries. The observation 'Nell logs (prepared IMlen the ~lls were drilled) show the till to be 40 feet thick, and the sand aquifer to extend from the base of the till to a depth of 75 feet IMlere it overlies the essentially impermeable bedrock shale. The valley has been cut into this shale bedrock and the flood plain sediments are approximately 1500 feet wide in this area. One observation well show.:; the potentiometric surface 15 feet below the surface, and the other shows it at 30 feet below the surface. The hydraulic conductivity of the clean sand aquifer is 1000 gal/day/ft2.
Although flow occurs across the unit boundaries bet\Neen the confining units and the aquifer, one can often ignore these flows because aquifer flows are so much greater. The following variables are knowi and can be plugged into Darcy's Law:
Aquifer cross-sectional area = 1500 ft X (75 ft - 40 ft) = 1500 ft x 35 ft.
A = 52,500 ft2 change in the potentiometric surface I = (30 ft - 15 ft)/ 5280 ft
The aquifer is saturated, since "potentiometric surface" data given
Q = (1000 gal/day/ft2) X ( 0.0028) X 52,500 tt2 Q =approximately 149, 150 gal/day
Fig. 21: Oblique and transparent view of valley sediments and geometry for Part B. Sediments are horizontal.
Page 35
UNITA
EXERCISE A2: The Relationship Between Shallow Water Level Contours and Flow Direction
Introduction Shallow water-level contours, also called equipotential lines, showthe distribution of
water in an aquifer at varying hydraulic heads (potential well-heights). Water in areas Vlklere the potentiometric surface is higher \Nill move towards areas Vlklere it is lower. Since ground-water flow occurs between areas of differing heads, there is no flow parallel to equipotential lines. The hydraulic gradient exists perpendicular to equipotential lines and flow occurs perpendicular them. Flow occurs in 3 dimensions, and equipotential lines are actually curving surfaces, but appear as lines Vlklen studied from the direction perpendicular to flow.
Objective The objective is to gain a better understanding of how the potentiometric surface can be
graphically presented and Vlklat other information can be obtained from that display. The relationship between the potentiometric surface elevation, hydraulic gradient, and the direction of ground-water flow \Nill be investigated. This exercise is a classic three-point problem, typical of one found in structural geology.
Supplies and Equipment Required Ruler INith metric and inch scales, protractor, calculator, notebook paper, and pencil.
Task Find the shallow water level contours between 3 observation wells, determine water
level contours and the local flow direction, and mathematically calculate hydraulic gradient.
Method Determine the water level in 3 observation wells under stable conditions. This water
level must be corrected for any variations in the surface elevations at the wells if the area under study is not perfectly flat. The water level (level of the potentiometric surface) in this case is given as elevation above mean sea level (MSL).
1) Straight lines have been drallVll connecting the 3 wells (seen as points) on a map. The result \Nill is a triangle.
2) Determine the drop in elevation (hydraulic head) between the 3 wells. There \Nill be 3 different numbers, each the number of feet difference measured along the connecting lines. These numbers should be \Mitten next to their representative
connecting line. These numbers are the number of imaginary contour lines (at 1 foot intervals) that cross this particular connecting line. We \Nill only draw the contour lines at 5 foot intervals.
3) A graphical method has been used to divide each connecting lines into the same number of equal segments as there are feet of head drop between well on each connecting line. A line perpendicular to a connecting line is dra11V11 from each of the well points away from the triangle, but only 1 line per connecting line.
3) A convenient ruler measure is picked that \Nill span from the well point opposite of a perpendicular line, to the perpendicular line (this is the scale line). This scale line is necessarily longer than the connecting line it \Nill be dividing into equal segments. In this case the centimeter scale was used, and either the centimeter or halfcentimeter marks were chosen (to match the number of feet head drop). There are three additional triangles now lying outside of the original 3 well point triangle.
Page 36
4) All the ruler marks are marked v.1th a tick on the scale line. There are as many tick marks as number of feet head drop betvveen the 2 vvells W"lose connecting line is being prepared for contour marking. Each tick mark representing a specified contour interval are marked darker. Marking of contour intervals can begin at either vvell point; the net result must be the same.
5) The scale markings are made on the scale line have been transferred back to the connecting line by laying a ruler perpendicular to the original connecting line across to each scale line darker (contour interval) tick mark. Only the portion W"lere the ruler crosses the connecting line is marked on the connecting line.
6) The corresponding contour inteNal can be Vlnitten dowi next to the tick marks transferred to the connecting lines. When this is completed there v-.111 be 2 contour elevations, 1 each on a different connecting line. These represent points of equal elevation on the potentiometric surface. Therefore they can be connected by a darker line passing through each point. There VIAii be a corresponding contour interval mark on another connecting line for each contour interval mark. Connect all points up to their matching point. A pattern should immediately become apparent: All equipotential (water-level contour} lines are parallel to one another. These represent the surface in much the same way as do topographic lines on a surface map.
7) The ground-water flow direction is in the down-gradient direction perpendicular to an equipotential line. These are all parallel. Draw the line for the flow arrow (including arroW"lead) near the center of the original triangle, perpendicular to elevation contour lines. The north direction arrow can be extended downward and the bearing (angle betvveen the flow direction arrow and north) can be measured.
The v...orksheet and solution answer sheet, shov.1ng connecting line division units and methods, equipotential lines, and the flow direction, are on the followng pages.
Direction of Ground-· I · Zl.6 "'"" Vvater Movement ~ "'-- ~/a~er Table Altitude
27.5--\- ---t --
Zl.2
26.8
Figure 22: Plan view of 3 well points v.1th water elevation data. Water table contours have been mapped and the flow direction drawn in (after U.S. EPA, 1987)
VJdl B Lf 31 h
Page 37
UNIT A I EXERCISE A2: Shallow Water Level Contours and Flow Direction Figure 23: Worksheet for Drafting of Equipotential Lines and Flow Direction
UNIT A/ EXERCISE A2: Shallow water Level Contours and Flow Direction
vue.11 B~ y31 f.t.
Ii CVVI
I 2. J.;"~s\01115-
f"ic:...1:::5 OV\. Q. 5 Ulo\,
N
Answer Sheet Showing: Connecting Line Division Units and Methods Equipotential Lines Flow Direction
I
I I
I
I
20 d;vi5iOV\~ /0 C..M
tic..\.<."'-"'~ o.!;,
Page 39
UNIT A
EXERCISE A3: Mapping the Potentiometric Surface
Introduction An understanding of the potentiometric surface is crucial for further study of ground
water and subsurface contaminants.
Objective This exercise attempts to bolster understanding of the concepts of potentiometric
surface and water table by having you draw a potentiometric map using water-elevation data from a number of observation 1t11ells and several surface water bodies. The folloiMng rules regarding equipotential lines must be follo~d if an accurate map is to be constructed:
1) equipotential lines do not cross 2) equipotential lines do not originate from the center of a map, but only at the boundary areas
of the map. 3) if an equipotential line does not intersect a boundary it must create an enclosed
shape; the line must be connected to itself 'Nith no breaks (see #2 above).
Supplies and Equipment Required Pencil and eraser
Task Generate a potentiometric map using the static \Nell-water level data listed next to the
\Nell points draVV11 on the folloiMng sheet. The contour interval is 5 feet. The wells are observation 1t11ells, or 1Nells IMlere pumping was stopped and a steady water level achieved before the measurements were taken. The data are given in elevation above sea level so that variations in surface elevations were factored out.
The rules governing potentiometric lines are listed above. Figure 25 shovvs a sample map as an example. The position of a equipotential line bet1t11een 2 ~II points only occurs if a contour interval falls somelMlere bet1t11een their respective elevations. If this criterion is met, the closeness of the line to 1 well point versus another should be a best estimate of the process follo1t11ed in Exercise A2. However, the contour lines '1.111 not be straight lines, because this map covers a much broader area typical of a hydrological site study.
Fig.25: Sample potentiometric map illustrating properties of potentiometric lines and sho'Ning \Nell point v.ater elevation data and contour lines proportionally spaced per well data.
I I
I
}
I I
I 1· Cf2G.
\ Lo.~OOll\~ ~ E t ~ v. Cf ) \of f-.t.. --
\
\ \
' \
Page 40
Worksheet for Unit A I Exercise A3 \
\ \ • 9 '2-f
• Cf 17
• 'to7
• 89Z
• 88'1
'
/
' ' ' /
/
/
)
\
' ' ' ......... • Cf 01
• 899
Figure 26: Worksheet for Unit A I Exercise A3. Map view of observation well water level data, given as elevation above sea level. Aquifer boundary conditions are sho'Ml.
--
L~~OOIJ\~
E ! ~ v. 't 1 '-f h.
I
I
l I
I. ~2C.
//
/
Page 41
Answer Sheet for Unit A I Exercise /:1:3
/
' /
/
)
.._ ' -·-..... ' ........... •'101 -~
• 899
16 890 ....____
.lrfl-l- .. -· ~ . . . - .... );::J.Jt ---~~---.
~-~ =~--- - --:-· >114-__
Figure 27: Answer sheet for Unit A I Exercise A3. Map view of observation well points and shallow water level contours dra'Ml in, describing the potentiometric surface.
Page 42
Appendix II
Exercises for Unit B
Page 43
UNIT B
EXERCISE 81: Contaminant Plume Movement
Introduction The concept of how quantitative values for porosity affect calculations involving the
actual measured (quantitative) value for porosity vvill be introduced here. Actually, flow through rocks or soils only occurs between grains of geologic material, not though the grains or particles. This flow is called interstitial flow and is determined by the effective porosity.
Effective porosity is the percent of the total volume of a given mass of rock or soil that consists of interconnecting pores or voids. A pore is not a conduit for flow if it does not communicate vvith adjacent pores, if those pores do not interconnect vvith others, and so on. For net flow (advection) to occur pores must interconnect, however tortuous the flow path may be.
Objective The objective is to see how the rate of movement of a contaminant plume can be
calculated and to examine the roll that effective porosity, a measurable (and someYIAlat predictable) quantity, plays in predicting the rate of movement of a contaminant plume.
Supplies and Equipment Required Calculator, pencil, and notepaper.
Task Read through the follovving contaminant release scenario and assemble the data
required to operate the equation and calculate the time required for the plume to reach the next well. This problem is from the U.S. EPA, 1987.
A conservative substance, chloride in this case, has been spilled. The waste liquid has infiltrated the unsaturated zone and begun dissolving into the aquifer water table. The aquifer consists of sand and gravel vvith a hydraulic conductivity of 2,000 gal/d/ft2 and an effective porosity of 0.20. The water table in a well adjacent to the spill site is at an elevation of 1,525 feet. A well one mile directly doV1111gradient has a static water level of 1,515 feet.
Determine the velocity of the water and contaminant (assume virtually no dispersion}, and how long it vvill be before the second well is contaminated by chloride. A modified form of Darcy's Lawvvill be used, vvith the conversion constant for converting gallons to cubic feet: 7.48 n3 per gallon. The modified formula for velocity is v =Kl/ 7.48n.
Where v = interstitial velocity n = effective porosity K = hydraulic conductivity I = hydraulic gradient
The scenario is illustrated in the cross sectional diagram (Figure 28) on the next page, along vvith the solutions and calculations.
Page 45
UNIT B
EXERCISE 82: Contaminant Plume Shapes
Introduction The shape of a contaminant plume depends on a variety of factors. The text has
concentrated on advection, dispersion, the type of contaminant, and the retardation processes. Another important factor is the length of time and any interruptions in the spillage or leakage of contaminant to the subsurface. Refer back to Unit B, Figures 10 and 16, a and b, to review helpful information that has been presented previously.
Objective Illustrate some of the temporal (time) factors affecting contaminant releases and how
they can be manifest in plume shapes.
Supplies and Equipment Required Pencil or pen
Task Match the four folloiMng contaminant plume shapes to the sets of possible causes listed
below in Figure 29. The ansv-.iers are given on the folloiMng page in Figure 30.
~ - u: 0 ... c !'l
,Q ~ 11 ' ... -0 ·- c 0 :> e
(.!)
Plume#1
Enlarging Plume
1. Essentially same waste input
2. SorptiOll capacity not fully utilized
3. Dilution effect fairly stable
4. Slight water-table f luctua:ion or effects of wa:er-table fluctuation not impertant
Plume#2
I ,' \
\, ! \ I \ I '~
Reducing Plume
Intermittent or seasonal source
Plume #3 Plume #4 Plume#5
:{ \ '.''' Contaminated zone Former boundary Present boundary
• Waste site
,... :'@:·ii:- \ I ·:: I I :,: I
I I I I I I
' I '-/
Nearly Stable S~runken Plume Plume
.SST C...
1. Increase in rate of discharged wastes
2. Sorption activity used up
3. Effects of changes in water table
1. Reduction in wastes 2. Effects of changes in
water table 3 More effective
sorption o<. More effective
dilution S. Slower movement
and more time for decay
& I I '\ I ,,
A v A \3
Series of Plumes
War..e no longer dis;xised and no lo~r leached a: abai doned was:e site
Figure 29 Plan view illustrating possible plume size and shape fluctuations due to various factors {after U.S. EPA, 1987, modified from U.S. EPA, 1977)
~ .... iI: 0 .... c ~ .g ~ ~ ' .... -0 ·- c 0 ::;J
e <!)
Plume#1
Eniarging Plume
1. Increase in rate of discharged wastes
2. Sorption activity used up
3. Effects of changes in water table
Page 46
EXERCISE 82: Contaminant Plume Shapes Ans1Ners to exercise on follov-Ang page
Plume#2
Reducing Plume
1. Reduction in wastes 2 . Effects of changes in
water table 3 . More effective
sorption 4 . More effective
dilution 5. Slower movement
and more t ime for decay
SET A
Plume#3
:H!.\:~:":i Contaminated zone F<>mler boundary Present boundary
• Waste site
Nearly Stable P;ume
1. Essentia:ly same waste input
2. Sorptiotl capacity not fully utilized
3. Dilution effect fairly stable
4. Slight v.ater-table fluctuation or effects of wa:er·table fluctuation not important
SE"T D
Plume#4
,... /®.\ : \@ : I I I I \ I
' I ..... _,,
Shrunken Plume
Waste no longer disposed and no longer leached at abandoned waste site
Plume#5
.. I I I I ,,
A\ VJ
@ Series of Plumes
Intermittent or seasonal source
SET'B
Figure 30: Plan view illustrating possible plume size and shape fluctuations due to various factors (after U.S.EPA, 1987, modified from U.S. EP.L .. 1977).
Discussion The enlarging plume is evidence of increased amounts of contaminants being entrained
into the ground vvater. This can be due to reduced release of conta11inants, just as an increasing contaminant amounts could reflect increasing release.
Water table elevation affects the amount of contaminant ossolving into it in the followng manner: Contaminants can be present in residual saturafon amounts in the unsaturated zone. For this part of a contaminant release to reach t'le vvater table, vvater {from either infiltration or water table level rise) must come into contact and dissolve the soluble portions of the plume. If the water table falls, the dissolved plume can be expected to become smaller.
A stable plume reflects stable conditions, v.tiile a shrunken plume indicates that methods to reduce the contamination are y..orking, or that the contaminant releases have stopped. The intermittent plume indicates periodic releases, rather than contimrus release. This can be due to human factors {eg. an industrial operation performed only once a )·ear) or can be the result of yearty variations in rainfall infiltration or major vvater table changes.
Page 47
UNIT B
EXERCISE 83: Remediation Problems and Strategies for NAPLs
Introduction This exercise investigates several NAPL plume physical properties in the subsurface. As
discussed before, NAPL contaminants present different and very difficult set of problems regarding containment and cleanup.
Objective Review the figures included llVithin this exercise concerning NAP Ls and DNAPLs. Study
the schematic of a NAPL release site and generate a possible scenario of plume movement, and list possible methods for dealing llVith the contamination.
Supplies and Equipment Required
Tasks Study Figure 31. The left-hand storage tank contains DNAPL, llVith a density greater than
that of water. The right-hand tank contains LNAPL, having a density less than water. The releases are due to leaks in the respective storage tanks. Note the geometry of the confining bed below the aquifer and the ground-water flow direction. Sketch the possible paths. shapes. and final location of the LNAPL dissolved and free-product plumes on Figure 32. Assume that a large amount of material was released over time. Review of Figures 33 through 37 concerning DNAPL plume behavior in the subsurface \/Viii provide hints as to the possible plume behavior.
Questions
1) What problems might be encountered during a site assessment?
2) What IM:>uld happen if the confining bed shown at the bottom 1Nere much deeper?
3) What methods of containment or remediation might be used to combat this environmental problem?
The ans\Ner keys are on the follollVing pages.
Page 48
EXERCISE 83: Remediation Problems and Strategies for NAPLs Diagram showing ans'Ner for plume sketch problem
Unsaturated Zone
- + --. - Water Table ---
DI r-ec.+-i'P"' er\: 0.-...,,,,,..6- wc::t-+~
~\ .. ..v
Source of Product
''""""' "'"\Th" w .... , Source of Product (Lesser Density Than Water)
--. --- -- ,, --
Figure 31: Worksheet sho""1ng cross section of aquifer, v.rater table, and ground-water flow for Exercise 83 (after U.S. EPA, 1987).
---
Unsaturated Zone
Page 49
EXERCISE 83: Remediation Problems and Strategies for NAPLs Diagram showing answer for plume sketch problem
Source of Product (Greater Density Than Water) Source :if Product
Figure 32: The possible shape for the contaminant plumes are shO\'KI (U.S. EPA, 1987).
Page 50
Answers to Questions for Scenario in Exercise 83:
1) What problems might be encountered during a site assessment?
NAPLs may not be suspected as the source of dissolved contamination. The plume
could be contributed to the V11rong source if the tanks shoVllll are on a large industrial site with
many other chemicals in use. If the DNAPL and LNAPL contribute some of the same dissolved
compounds to the aquifer, only one NAPL might be suspected and remediation centered on only
the one type. The pools that form v-..tlen a large quantity reaches (and penetrates, in the case of
DNAPL) the water table may not be found in a limited evaluation using only a few observation
wells. The DNAPL plume could be mistaken to be traveling in the direction of local ground-water
flow, rather than doVllll the slope of the confining bed.
2) What v.ould happen if the confining bed shoVllll at the bottom were much deeper?
The confining bed serves to keep the plume from penetrating deeper into the
subsurface. Plumes are generally easier to control and remediate v-..tien they are closer to the
surface. For example, subsurface barriers can only be installed up to a certain depth. A deep
penetrating plume has a better chance for contaminating regional ground-water flow and moving
greater distances. This usually means off the contaminant release site and perhaps into more
sensitive areas or surface bodies of water (U.S. EPA, 1991)
3) What methods of containment or remediation might be used to combat this environmental
problem?
The initial approach v.ould be to prevent the spread of the free-phase product, thereby
reducing the amount of aquifer material contaminated to residual saturation levels. If the
confining bed is close enough to the surface (per the claims of the manufacturer), a subsurface
barrier could be installed to stop the DNAPL plume from moving doV1111-slope. This barrier might
also be able to block ground-water flow into the plume area, reducing the amount of dissolved
contaminant spreading away from the main plume. The barriers v.ould probably be used in
conjunction with hydrodynamic controls to ensure containment. Barriers might be used primarily
to control movement of uncontaminated water into the plume area. If barriers were impractical,
hydrodynamic controls v.ould be the only means to control movement of the plume.
There is the chance that active withdrawal and treatment (pump-and-treat) could be
practical for the site. In this case an attempt v.ould be made to access the free-product pools as
well as the dissolved phase and soil gases (if any).
Page 51
Residual Saturation of DNAPL in Soil From S~
J F---2~-----~r:m':;:]lG,lnfiltration and
Leaching
Figure 33: DNAPL of insufficient volume to completely saturate the unsaturated zone and reach the water table. DNAPL mass is exhausted before free-product phase reaches the water table, but soluble components are able to contaminate ground water (U.S. EPA, 1991).
Vadose
-
Residi.al Satvraticll of
DNAPL in Soil f FromSpill
Residual Saturation in Satu'ated Zone
Figure 34: DNAPL release of sufficient volume to overcome residual saturation in the unsaturated zone and consequently penetrate the water table (U.S. EPA, 1991 ).
C<ihllni1n--:.:-:-.· -
Figure 35: Migration of DNAPL through the unsaturated zone to an impermeable boundary (U.S. EPA, 1991).
)'::/\,, ... ,... Low Permeable -Stratigraphic Unit
CLAY
Figure 36: DNAPL in free-product form as a perched reseNoir (U.S. EPA, 1991 ).
Ground111ater Flow
Figure 37: Confining bed tipped geometry causing flow of DNAPL in direction different than that of ground-water flow. Note that the dissolved plume movement is iMthin the ground-water flow(U.S. EPA, 1991).
Page 53
Appendix Ill
Glossary
advection - flow of ground water and/or contaminants due to hydraulic gradient and gravity. The dominant transport process for ground water and all soluble contaminants.
aeration, zone of - (see unsaturated zone)
capillary fringe - the volume of material located just above the saturated zone. It is saturated, but at negative atmospheric pressure, in place due to the vvicking action of pores
contaminants - all physical (including radioisotopes and biological particles) and chemical solutes introduced into the hydrogeologic environment due to human activity (after Freeze and Cherry, 1979); can come from both natural and man-made sources;are considered "pollution" Wien concentration increases above a certain level (quality standard).
DNAPL - an acronym for "dense nonaqueous-phase liquid", synonymous vvith dense (relative to water) immiscible-phase liquid (hydrocarbon). The movement of DNAPLs in the subsurface is difficult to predict, as their movement is determined by properties different from those of ground water (see NAPL).
density - the mass (or weight) of a substance per unit volume, Wiich can also be expressed as a (unitless) ratio as compared to water, eg. a compound having a ratio of 1.15 is denser than water (vvith a density of 1.00) and 11\,{)Uld sink.
diffusion (molecular diffusion) - the spreading out of molecules or ions into a fluid or porous medium in a direction tending to equalize concentrations in all parts of the system. [Produced by differences in chemical concentrations Wiich tend to be erased in time by random molecular motion; 11\,{)rks together vvith dispersion.]
dispersion (hydrodynamic dispersion) - spreading of a plume produced by natural differences in local ground-water velocities related to local differences in permeabilities. [Works together vvith diffusion.]
discharge - the loss of water from an aquifer or zone of saturation, such as vvithdrawal, draining, evapotranspration, seepage, etc.
discharge rate - stream flow, well flow. [units are a volume (or quantity) per unit time, such as gallons per minute (gpm).]
dra'M:lov-.11 - the lowering in height of the water table (and water level in a well) on a local or regional scale due to pumpage (vvithdrawal) from an aquifer; a measure of height {length), the reduction in hydraulic head due to vvithdrawal of water from a well.
ground-water flux rate - flow rate per unit area; a discharge rate, also knov-.11 as the bulk flow rate [units are gal/day, symbol is Q.)
ground-water flow rate - volume of water flovving, units are gal/day.
Page 54
hydraulic conductivity - a measure of the ability of medium to transmit water, units are fUday [also gal/day/ft2], symbol is Kor p. Permeability is a qualitative term for hydraulic conductivity.
hydraulic gradient - the slope of the water table or potentiometric surface, the change per unit distance, the driving force for ground-water movement. [Units are feet per foot, symbol is 1.)
hydraulic head - the difference in elevation of water level between tlM) points, given as distance unit; denotes pressure differences affecting flow in ground-water systems, [symbol is h.]
immiscible contaminant - a contaminant that is composed of entirely or predominantly immiscible (not mixing VI.1th water) liquids; forms a distinct boundary Wien mixing VI.1th water is attempted. However soluble components are able to dissolve into ground water (see NAPLs).
interstitial velocity - the velocity of water and/or contaminants in interconnected pores, taking into account that advection does not occur through the grains (solids).
ion exchange - the exchange of ions of a contaminanUground-water solution VI.1th geological materials present in the subsurface, usually controlled (and possibly reversed) by changes in pH and chemical conditions.
LNAPL - an acronym for "light nonaqueous-phase liquid", synonymous VI.1th less dense (relative to water) immiscible-phase liquid (see NAPL).
NAPL - acronym for nonaqueous-phase liquid; a hydrocarbon that Wien mixed VI.1th water results in a physical interface between the t\M) liquids. This interface divides the tlM) liquids, but compounds in the NAPL are not prevented from dissolving into ground water. [See dense NAPL (DNAPL) and light NAPL (LNAPL).]
partitioning - the entrapment of a portion of a NAPL in continuous-phase form in the pores of a geological material Wien in the presence of water. The NAPL becomes immobile in the small pores, or in large pores Wien flow slows relative to that in smaller pores.
porosity - the ratio of open pore spaces in a rock or soil to its total volume, defines amount of water or liquid a rock can contain. [Expressed as a percentage or decimal fraction, symbol is e (theta), term is unitless.]
porosity, effective - the percent of the total volume of a given mass of rock or soil that consists of interconnecting pores or voids, symbol is n.
potentiometric surface - the water table surface or level (or potential surface, if not in a confined unit), can be expressed in graphical form as a potentiometric surface map of equipotential lines, similar to topographic lines; also called the piezometric surface.
recharge - the addition of water (refilling) to an aquifer or zone of saturation, such as rainwater infiltration, or seepage from a river or pond.
remediation - general term referring to activities undertaken to improve a contaminant problem and to prevent the IM)rsening (spread) of contamination.
Page 55
residual saturation (contaminant) - immiscible-phase liquid held on the pore spaces by capillary tension; cannot be mobilized by typical hydraulic forces (local ground-water flow)
residual saturation (water) - the amount of water remaining in the pore spaces of a material when the material is allowed to drain by gravity. This amount cannot decrease below a certain threshold amount
retardation - any one of several methods that can slow or temporarily stop the spread of contaminants in ground water in the subsurface. Includes partitioning, ion exchange, and sorption.
run-off - the moisture from precipitation that does not infiltrate (soak into) the ground because of saturated or special soils. Run-off instead flows over the surface. Run-off flows along drainages and low areas.
saturation zone (ground-water zone) - the zone below the water table; all pore spaces are filled Vllith water, contaminant, or water and contaminant
solubility - how easily a compound or component of a contaminant dissolves into water under "standard conditions", controlled by the polar character of the solute and solvent, pH, temperature, other chemicals present, etc. In general, the "heavier" and more complex contaminants have a lower solubility in water
sorption - when a dissolved ion or molecule becomes attached to the surface of a solid or dissolves in the solid; actually of tV1.0 types of processes: adsorption, a surficial phenomenon, and absorption, the phenomenon involving movement of material from solution to sites Vllithin the structure of the solid phase. These reactions are usually fast and reversible.
specific yield - the amount of water a rock releases if allowed to drain by gravity, which is not the total water the rock contains; the volume available for Vllithdrawal by wells.
unsaturated zone - the zone above the saturated zone (water table), which may contain saturated or partially saturated (Vllith water and/or contaminants) sediments; overlies the saturated zone, the contact area between the unsaturated zone and saturated zone is known as the capillary fringe. [Also known as the zone of aeration or the vadose zone.]
velocity, interstitial (bulk velocity) - the flow of a particular front of water; how fast an advective front moves; affected by the effective porosity, hydraulic conductivity, and hydraulic gradient. [units are fUday, symbol is v.]
water table - the surface of the upper limit of the saturation zone in an unconfined aquifer, given as an elevation above sea level or a distance below the ground surface. [Units are in length (see potentiometric and piezometric surface).]
Vllithdrawal rate - the rate at which water is removed or pumped from an aquifer via a well, or series of wells; expressed as a volume per unit time.
Page 56
References Cited in Text and Captions
U.S. EPA, March 1987, Handbook: Ground Water, EPA/625/6-87/016, U.S. Environmental
Protection Agency, Office of Research and Development
U.S. EPA, September 1989, Seminar Publication: Transport and Fate of Contaminants in the
Subsurface, EPA/625/4-89/019, U.S. Environmental Protection Agency, Center for
Environmental Research Information, Cincinnati, Ohio 45268, and Robert S. Kerr
Environmental Research Laboratory, Ada, Oklahoma, 74820
U.S. EPA, April 1991, Dense Nonaqueous Phase Liquids: A Workshop Summary, U.S.
Environmental Protection Agency, Robert S. Kerr Environmental Research Laboratory,
Ada, Oklahoma, Office of Research and Development
Page 57
References Cited in Captions Only
Freeze, R.A., and J.A. Cherry. 1979. Groundwater. Prentice Hall, EngleV>.Ood Cliffs, NJ.
Geraghty, J.J., and D.W. Miller. 1985. Fundamentals of Ground Water Contamination, Short
Course Notes. Geraghty and Miller, Inc., Syosset, NY.
Heath, RC. 1984. Ground-water Regions of the United States. U.S. Geological Survey - Water
Supply Paper 2242, U.S. Government Printing Office, Washington, DC.
Heath, RC. 1983. Basic Ground-water Hydrology. U.S. Geological Survey Water-supply Paper
2220, U.S. Government Printing Office, Washington, DC.
Huling, S. G., J. W. Weaver, March 1991. Dense Nonaqueous Phase Liquids, in U.S.